As To Spaces From Different Universal Settings

Let us here consider two different orbifold eigensets -- one orbifold eigenset of which is to be from one universe, while the other orbifold eigenset is to be from another universe.  These two different given arbitrary respective orbifold eigensets, would then work to belong to two different respective universal settings.  This would then mean, that each of the two said different orbifold eigensets -- would here act as two different spaces -- that would then be of two different universal settings.  This would then mean, that each of the two said eigensets, is to not be of a Real Reimmanian nature towards the other of the two said orbifold eigensets.  This would then, as well, mean, that each of the two said eigensets is to be of a Njenhuis-based nature towards the other of the two said eigensets.  Yet, if there were to be a kinematic group-attractor, that is to be Yukawa upon both of the two said orbifold eigensets -- that is to work as a holonomic substrate that is to be kinematic here upon the so-eluded-to proximal locus, as a physically taken eigenbase -- in relation to what would here be a relative Fourier-initiated Gaussian-based assortment of one of the two so-stated orbifold eigensets when this is in relation to the other of the two so-stated orbifold eigensets, then, this general genus of a Fourier-initiated Gaussian-based assortment, may often act in such a manner in so as to work to cause -- what would here be the equivalent of a physically-based Li-Algebra-related eigenbase, in so as to be able to help in so as to make both of the two so-stated orbifold eigensets, to then be of the same universal setting, over a successive series of group-related instantons -- that would take part in such a so-eluded-to group-metric.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Converging Phenomena From Parallel Universes

Let us initially consider a set of many orbifold eigensets, that are each individually taken -- as distinct given arbitrary respective orbifold eigensets, that are each from different universal based settings.  Let us say, that -- for each of the said orbifold eigensets that are each from different universes -- there is a Hamiltonian operator that acts as a group-attractor, that all work to pull each of these said individually taken sets of superstrings that operate in so as to perform one specific function, per each of the said individually taken orbifold eigensets -- in a manner that works in so as to pull the holonomic substrate of the said orbifold eigensets together, into a proximal localized set region -- that is of a relatively tight Laplacian-based setting, over a relatively transient duration of time.  Let us then consider such an interaction, as the Fourier-based activity of the kinematic motion of a certain set of orbifolds, that are initially relatively spatially separated -- to be brought into the same general substringular region -- by the Fourier-based activity of a separate physical entity, that works to cause the Ward-Neumman constraints of each of the different given arbitrary individually taken orbifold eigensets, to be converged towards a region that is much more proximal and of a localized conformally invariant-based setting.  Let us next consider the condition that would exist, if each of the then brought relatively close together orbifold eigensets -- were to still each work to bear a different tense of a Gaussian-based Li-Algebra spatial-related setting.  This would mean, that -- although each of these said orbifold eigensets were to then be spatially convergent, in a relative tense, -- the Fourier-based activity of each of the said orbifold eigensets, would still not be viable upon each other, over a relatively transient duration of time.  To Be Continued!  Samuel David Roach.